SIMPLY SUPPORTED BEAMS 63
1.2 m
12 kN 400 N 20 kN
1.3 m 1.5 m
PQ
RP RQ
Figure 5.14
(a) At equilibrium,
RP+RQ= 12 + 0. 4 + 20
= 32 .4kN ( 1 )
Taking moments about P: clockwise mo-
ments=anticlockwise moments i.e.
( 12 × 1. 2 ) + ( 0. 4 × 2. 5 )
+ ( 20 × 3. 5 )
}
=(RQ× 5. 0 )
14. 4 + 1. 0 + 70. 0 = 5. 0 RQ
from which,
RQ=
85. 4
5. 0
= 17 .08 kN
From equation (1),
RP= 32. 4 −RQ= 32. 4 − 17. 08
= 15 .32 kN
(b) For the reactions of the supports to be equal,
RP=RQ=
32. 4
2
= 16 .2kN
Let the 12 kN load be at a distancedmetres
fromP (instead of at 1.2 m fromP). Taking
moments about pointPgives:
( 12 ×d)+( 0. 4 × 2. 5 )+( 20 × 3. 5 )= 5. 0 RQ
i.e. 12 d+ 1. 0 + 70. 0 = 5. 0 × 16. 2
and 12 d= 81. 0 − 71. 0
from which, d=
10. 0
12
= 0 .833 m
Hence the 12 kN load needs to be moved to a
position 833 mm fromPfor the reactions of the
supports to be equal(i.e. 367 mm to the left of its
original position).
Problem 10. A uniform steel girderABis
6.0 m long and has a mass equivalent to
4.0 kN acting at its centre. The girder rests
on two supports atCandBas shown in
Figure 5.15. A point load of 20.0 kN is
attached to the beam as shown. Determine
the value of the forceFthat causes the beam
to just lift off the supportB.
F
3.0 m 1.0 m
4.0 kN 20.0 kN
2.5 m
A C B
RC RB
Figure 5.15
At equilibrium,RC+RB=F+ 4. 0 + 20 .0.
When the beam is just lifting off of the supportB,
thenRB=0, henceRC=(F+ 24. 0 )kN.
Taking moments aboutA:
Clockwise moments=anticlockwise moments
i.e. ( 4. 0 × 3. 0 )+( 5. 0 × 20. 0 )=(RC× 2. 5 )
+(RB× 6. 0 )
i.e. 12. 0 + 100. 0 =(F+ 24. 0 )× 2. 5
+( 0 )
i.e.
112. 0
2. 5
=(F+ 24. 0 )
from which, F= 44. 8 − 24. 0
= 20 .8kN
i.e.the value of forceFwhich causes the beam
to just lift off the supportBis 20.8 kN.
Now try the following exercise
Exercise 27 Further problems on simply
supported beams having
point loads
- Calculate the force RA and distance d
for the beam shown in Figure 5.16. The
mass of the beam should be neglected and
equilibrium conditions assumed.
[2 kN, 24 mm]